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10:00 PM
More fun when you're in free space, of course. Then it's just $dF=0$ as well.
 
@Ted hi, perhaps you know how to solve this ?
 
When is the similarity class of a real matricx $A$ closed ? $A$ has to be diagonalizable, but is that sufficient ?
 
Hm, I'm forgetting. Is the form version of $F^{\mu\nu}=\partial^\mu A^\nu -\partial^\nu A^\mu$ just $F=dA$?
 
Closed topologically in the space of matrices?
Yes, @Semiclassic.
Salut, Dodo.
 
Mmkay, I figured.
 
10:02 PM
Yes @Ted
 
In QCD I know one has additional terms in $F^{\mu \nu}$ but I forget what they are.
Something something covariant derivative, maybe.
 
Dodo, that's a usual trick where you add extra variables.
@Semiclassic, now you sound like Danu.
 
@TedShifrin Nah. I'll bunk school tomorrow.
 
@Astyx: Seems like it is sufficient. What're you thinking?
 
10:06 PM
found it on wikipedia. you get an extra term proportional to $i[A^\mu,A^\nu]$.
 
@Semiclassic: That's not covariant derivative.
Oh, well, is $A$ supposed to represent a connection? Then it might be.
 
Yeah.
 
Right, $d+A$ is the connection.
 
In that context, $A$ and $F$ are supposed to have 'color' indices as well. So $A$ needn't commute with itself.
 
Of course not.
 
10:08 PM
Well, in electrodynamics it would since it's just a single scalar field.
 
$U(1)$ is abelian, yeah.
 
I wonder if I can get myself to jumpstart on some foliation theory
 
@Astyx: So you've now learned Jordan canonical form, I take it?
 
The wiki article does give the covariant derivative version, namely $F_{\mu \nu}=[D_\mu,D_\nu]$ up to an overall constant.
They also give a differential-forms way of writing it. $\mathbf{G}=d\mathbf{\mathcal{A}}+\mathbf{\mathcal{A}}\wedge \mathbf{\mathcal{A}}$
 
Well I have the proof with complex matrices.
I was wondering if it held that since two real matrices that are similar in $M_n(\Bbb C)$ are similar in $M_n(\Bbb R)$ and since $M_n(\Bbb R)$ is closed in $\Bbb M_n(\Bbb C)$, then it follows that $Sim(M)$ is closed iff $M$ is diagonalizable in $M_n(\Bbb R)$, but I don't think that's enough.
(By the way, is diagonalizable the right term ? It seems really weird)
I guess it's true but to prove it one has to do the same proof as in $M_n(\Bbb C)$ all over again
 
10:12 PM
Which I guess goes with what you said above, since you can write $\mathbf{G}=(d+\mathcal{A})\wedge \mathcal{A}$?
 
@Ted I don't think I have, at least I don't know the name
 
So how do you know non-diagonalizable implies not closed?
 
Oh, I do have an actual question for you.
 
Aren't all square matrices similar to their Jordan decomposition?
 
Over an algebraically closed field?
@Semiclassic, actually the curvature should be $(d+\mathcal A)^2$, suitably interpreted.
 
10:15 PM
Hmm.
 
I mean, any square matrix can always be written as a block triangular matrix sandwiched between unitary matrices?
 
Suppose I have (as I said earlier, though with slightly different notation and in less generality) the affine curve $f(x,y)=(y-x)(x-x_1)(x-x_2)(x-x_3)=0$.
 
I have a proof where you take $D = Diag(1,2,\dots, n)$ and take $A$ triangular (which you can without leaving the similarity class in $M_n(\Bbb R)$) and then compute $D^kAD^{-k}$. This converges to $Diag(a_{1,1}, \dots, a_{n,n})$ which is by hypothesis in $Sim(A)$. The result follows
I don't think we're going to study Jordan canonical form this year
 
As a projective variety, there'll be 3 Riemann spheres with a common (triple) point and another Riemann sphere which shares double points with the others.
 
Where are you using non-diagonalizable, then, @Astyx?
Right, @Semiclassic.
 
10:18 PM
First question: How can a triple point resolve?
 
I proved the contrapositive @Ted
 
With a double point I expect to replace the node with a handle.
 
To think about the converse, I think you need Jordan form.
 
But I'm not sure what can happen with a triple point.
 
Right, @Semiclassic. You're unpinching a pinched torus.
 
10:19 PM
Right.
 
Triple point comes from higher genus.
But if you wiggle it you should get 3 nodes nearby.
So it's like starting with 6 nodes.
 
The converse can be solved using minimal and caracteristic polynomials
 
Understanding minimal polynomials is a good part of Jordan form, @Astyx.
 
I'm not really following what is meant by 'wiggling.'
Though I presume it amounts to a certain perturbation.
 
10:21 PM
Generic small deformation.
 
Then when $A$ is diagonalizable, it follows that $Sim(A) = \chi^{-1}(\{\chi_A\})\cap \mu_A^{-1}(\{0\})$
 
I have no idea what that means, @Astyx.
 
Oh, I think I see what you mean (maybe).
I start with a triple point, but if I wiggle then I can replace that triple point with another Riemann sphere which touches the others in nodes.
And then if I perturb that, I get handles.
 
Oh sorry, $\chi : A \mapsto \chi_A$ is the function that maps a matrix to its caractristic polynomial, and $\mu_A$ is the minimal polynomial of $A$. And $Sim(A)$ the similarity class of $A$
I might be using Jordan form without knowing it
 
The difficulty in my case is that my perturbation is not generic: $f(x,y)\to f_t(x,y)=(y-x)(x-x_1)(x-x_2)(x-x_3)-t(x-x_1)(x-x_2)=0$.
 
10:24 PM
It still doesn't make sense. You need functions on the space of matrices. So what you're writing down isn't right.
 
(I really have 3 such perturbations, but their coefficients are independent so I wanted to start with that one.)
 
Do you mean me @Ted ?
 
Yes.
 
My functions are on the space of matrices, are they not ?
 
What I want to say is that I can rewrite the perturbed curve as $[(y-x)(x-x_3)-t](x-x_1)(x-x_2)=0$.
 
10:27 PM
So just as a double point drops genus by 1, a triple point drops it by 3.
 
Problem is, I don't know how that affects the triple point.
 
@Astyx: I think you mean $\mu^{-1}(\{\mu(A)\})$ or something.
Well, write than down carefully in homogeneous coordinates, @Semisimple.
 
Heh.
Fair enough.
 
The $t$ needs a $z^2$.
 
Well, I'm only writing down the affine curve.
If I want the projective one, the x_k's also need z's.
 
10:29 PM
Yes.
 
What I really want, at the end of the day, is three such perturbations.
 
Hold on and figure out one.
 
$\mu$ is not continuous, so that wouldn't work. I mean $$\mu_A : \begin{cases}M_n(\Bbb K) \mapsto M_n(\Bbb K)\\B \mapsto \mu_A(B)\end{cases}$$
 
Yeah.
 
OK, I cannot multitask any more.
 
10:31 PM
I'll leave then :)
I need to sleep anyways
Bye !
 
Main reason I mention that is because I can write the general case as $$y=x+\frac{t_1}{x-x_1}+\frac{t_2}{x-x_2}+\frac{t_3}{x-x_3}$$
 
And thanks
 
Bye.
 
(or as many as I want, really).
 
Semiclassic. Quit it. Focus.
That perturbation doesn't move anything at infinity.
 
10:33 PM
@Semiclassical A link of the triple point looks like a Hopf linkage. Three circles, each linked to each other by linking number 1.
 
Hmm, then maybe I'm making things more complicated than I should.
 
You cut out the singular interior and glue back it's Siefert surface.
 
Does that explain why normalization adds 3 to the genus?
its
Balarka, of course we're trying to stay in the algebraic category here ...
 
What I say can be done algebraically, I am quite sure.
 
Well, I'm resolving the triple point into three nodes ... then resolving them.
 
10:35 PM
Because what you do for a node is exactly what I say; cut out the singular interior of the Hopf link and glue back it's Siefert surface. That's going from $z_1z_2 = 0$ to $z_1z_2 = \epsilon$.
 
Hmm, it looks like $(y-x)(x-x_1 z)-tz^2=0$ has no singularities (for $t\neq 0$.)
 
@TedShifrin That's also a possible thing to do. Do we end up with the same genus?
Yours add 3...
 
Right, and that's what a triple point should do. Do you see it your way?
 
you = ?
 
You should learn about Milnor fibers. There's another cool Milnor book for you to read, Balarka.
 
10:37 PM
What's the genus of the Siefert surface of three circles with each pair linked by linking number 1? I wonder if it's 3.
 
That's too much topology for me :P
 
I'm okay with not talking about milnor fibers atm :)
 
I'm talking to Balarka, not you.
 
@TedShifrin Ah, yeah, I have heard of it.
 
Hence why I asked "you = ?" :P
 
10:39 PM
I'm just saying that in your original, setting $z=0$ kills the $t$ term and so it does us no good for changing the triple point. Or am I missing something, @Semiclassic?
 
No, you're probably right.
 
hi chat , how to find the intersection of 2 surfaces in space ? am doing stokes theorem
 
So I shouldn't expect this perturbation to affect the singularities at infinity whatsoever (?).
 
Too vague a question, Kasmir.
 
ill write on latex and post an example
 
10:41 PM
is there a name for an inner product which is positive semidefinite instead of positive definite?
 
Well, the point $[0,1,0]$ is still on those curves for all $t$, @Semiclassic.
 
usually a degenerate inner product, @Alessandro. I dunno.
 
One other thing I'm interested in, and this is where I get confused, is that if I consider the one-form $y\,dx$
 
$x^2+y^2+z^2 =1$ and $x+y+z=0$ , $z=-x-y$ --> $x^2+y^2+xy =1/2$
 
10:42 PM
I do examples like that in my lectures, @Kasmir.
 
then when I've got $y=x+\frac{t}{x-x_1}$ then it'll have a pole at $x=x_1$ whenever $t\neq 0$.
 
Don't do so much algebra. You don't want to project to the $xy$-plane. You want to work in the plane $x+y+z=0$. @Kasmir
 
hmm but i dont get the concept of that
 
(I, by contrast, probably shouldn't be projecting onto the xy plane so much.)
 
how does the condition of unit sphere play roll here?
 
10:43 PM
Depends on the problem, @Kasmir, but I gave my students lots like that where you should just figure out $\text{curl} F\cdot n$ using the plane.
 
if all i care about is the plane $x+y+z=0$
okay ill watch that lecture now
 
It intersects the plane in a great circle. But that circle bounds a disk in the plane.
 
wha-oh, gotta catch the train
 
Bye, @Semiclassic. I'm not following you anyhow.
 
you use differentials to deal with surface integrals and you asked me not to do it that way
so i did not watch further =p
but I assume that strokes theorem cant be taught in one way right?
 
10:45 PM
I talked about interpreting it as a flux directly. What's your $F$?
 
F = ( 3y-2z , z-3x , 2x-y )
 
Right. Compute curl. It is a constant vector field. How do you calculate the flux across a region in the tilted plane? $\text{curl}\,F\cdot n$ will be a CONSTANT.
 
@TedShifrin Ya, it's 3.
 
Il ldo the curl now
but that is not where I have difficulty
its the set up again
 
Had to be, @Balarka. I have no idea why, but it had to be :)
I'm saying that you need to think, @Kasmir, not grind formulas.
 
10:48 PM
I mean we have two surfaces and they intersect to form a closed curve
 
What's the integral of a constant over a circular region of radius $1$?
 
the area of it
pi
 
times the constant. Right. Done.
No horrible formulas. Just understanding what you're doing with the theorem.
 
(Caught the train in time, good thing I hurried)
 
IT's an excellent sort of homework and test question.
LOL @Semiclassic. You couldn't run all the way home?
 
10:49 PM
What does degree-genus say about it? 3 is the minimal possible genus, yeah?
I forgot the formula
 
Not when I'm living with parents in the suburbs.
I take a 20 minute light rail trip to St Paul, then a half hour bus ride to the northern suburbs
Can't run that :p
 
@TedShifrin how do you know that the plane intersects the sphere in a circular shape algebraiclly ?
because we deal also with many other surfaces that are hard to see
 
You don't see it algebraically unless you use linear algebra to change coordinates. You use geometry instead.
 
hmm okay =p so if I understood correctly now
r (x,y) = (x , y , -x-y )
 
Anyways. I suspect what I don't grok right now is how contour integrals over a projective curve in CP^2 and over the affine curve in C^2 are related.
I ultimately am interested in integrals on the curve rather than the curve itself.
 
10:55 PM
Don't do that, @Kasmir. You do NOT want to do it algebraically. You have to do it by thinking.
 
But I'm feeling pretty handwavy now
 
hmm am absoluley lost , the plane intersect the sphere in a circle right?
i need that information about circle becuse am gonna do surface integral
of that region
 
@Semiclassic: Your affine curve is the whole curve except for a finite number of points. The question is whether your 1-form has singularities there?
Read all the things I've said to you for the last 20 minutes, @Kasmir.
 
Ok I will , thanks :)
 
The other thing I'm getting mixed up on in practice are singularities of the curve versus those of the one-form
 
11:00 PM
The singularities of the curve shouldn't actually affect integrating the 1-form. If the path happens to go through a singular point, you pull back to a desingularization of the curve and you have no problem. I guess there are issues with what the 1-form means at such points.
 
Aren't you asleep, @Alessandro? :D
 
@TedShifrin so far am here double integral of surface , ( -2 , 4, -6 ) dot ( 1,1,1 ) normal of the plane
 
neither am I
 
UNIT normal, @Kasmir, UNIT normal.
 
11:04 PM
I'm insisting on doing this in a curve-centric way because ultimately I'll only have $y(x)$ by virtue of $f(x,y)=0$.
 
@TedShifrin oh yes >< sqrt3 , okay but ehm now my question is what is that surface
 
I'm about to go to sleep since the numerical analysis exam begins in 9 hours or so
Good night everyone
 
i know its a circle but what radius
 
It's the inside of the circle of radius 1 in the plane.
 
night
 
11:06 PM
It's radius 1 because the plane goes through the origin. If the plane didn't go through the origin, you'd need to use the Pythagorean Theorem to find its radius.
 
how do you know that?
 
Draw a picture and think.
 
hmm, I should read some of Ginsberg at some point.
 
Ok, out for now to avoid getting a headache from typing on mobile
 
@TedShifrin i see what you mean now
@TedShifrin because it goes through the origin it cuts the sphere into 2 equal pieces
but diagonally
 
11:08 PM
If I gave you the plane $x+y+z=1/2$, what would be the radius of the circle?
 
let me think
we shifted the plane by a 1/2
hmm I dont know how to do this geometrilly
but i assume i need to solve it for z and then plug in on the unit sphere
 
Draw a 2-dimensional cross-section of the picture. Circle, line ... How far is the line from the center of the circle?
 
r = 1/4
 
Hold on. You jumped to the end.
 
@TedShifrin the way i did it was to draw it on yz plane and found the y intersect
 
11:23 PM
I don't think that's right. The closest point to the origin on the plane won't be on the yz plane.
 
hmm why do we need to find the closest point ?
i found the diameter
and took half of it
 
Because the center of the circle will be the point on the plane closest to the center of the sphere (the origin).
 
y = 1/4 + sqrt (7/4) , 1/4 - (sqrt7) /4
 
No. Remember the normal to the plane is $(1,1,1)/\sqrt{3}$.
 
Can you show me how you thinking ?
 
11:30 PM
I want to find how far along $n=(1,1,1)/\sqrt3$ I have to travel to meet the plane. That point will be the center of the circle I'm looking for.
So I get a little right triangle — the distance I traveled and the radius of the circle are the legs of the right triangle, and a radius of the sphere (length 1) is the hypotenuse.
 
You use pytagoras ?
 
Eventually, yes.
But first you want to know for what value of $t$ you have $t(1,1,1)/\sqrt 3$ lying on the plane $x+y+z=1/2$.
 
hmm thats a smarter way of doing it
 
Part of what you need to learn is to visualize things and try to use concepts, not always horrible calculations.
 
well we did not do much of space geometry
 
mt3
11:33 PM
hello can somebody please tell me what the dimension of an open cover is?
 
so I have absolut no backround on it
 
No time like the present, @Kasmir :)
 
@TedShifrin I see how that would be usefull in the theorems am using but do you have videos from basic ?
we started with those theorems in space without any knowledge of space geometry
thats why I got lost
 
@mt3: Are you talking about covering dimension? You can read on Wikipedia, I'm sure.
 
mt3
oh i searched for it, but the term "Lebesgue" in the results put me off
 
11:36 PM
@Kasmir: There were lectures at the beginning of the course on projections and thinking about level curves and level surfaces. I don't think I ever did explicitly what we were just doing.
 
mt3
but apparently that is what i was looking for
thanks
 
@mt3: He's the one who came up with it.
 
@TedShifrin okay thanks alot Ted! you are the only person who can get this ideas into my head :D
 
But you should try to draw a picture looking at the plane on the edge ... so the normal is perpendicular and then you see the triangle we were just talking about. @Kasmir.
You should try discussing stuff with more of your friends taking the course, @Kasmir. Working together and teaching one another is a good thing.
 
@TedShifrin We do that :)
 
11:38 PM
Need to draw more pictures!! And make sure they make sense.
 
on some problems we have to find r (s,t) = (s,t,f(s,t))
and project the 3 d surface into st plane
and sometimes the geometry is too hard so that is why am trying to do all algebraiclly
 
You need to do lots of problems and figure out when to do what. Just like you did when you first learned to take integrals ...
OK, I'm gone now.
Have fun.
 
@TedShifrin okay thanks alot again :) bye :)
 
hey what the formula for computing general polynomial powers in a ring ?
 

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